594968 五、發明說明(1) (一)、【發明所屬之技術領域】 本發明係有關於半導體元件之製造,特別是關於—種 形成在積體電路製造中靜電放電(ESD)保護的NMOS元件之 方法。 (二)、【先前技術】 積體電路(ICs)容易受到稱為靜電放電(esd)現象損壞 的影響,於元件傳輸及處理期間當大靜電荷聚集於其^ ^ 針上時,會發生£^1)。若控制的不適當時,ESD將會無法挽 回地損壞1C,就如同在元件結構内放電產生大規模溫 斜期間功率的消散。 又 一個解決ESD的問題是,連接在1(:上靠近外部聊引接 合墊的矽控制整流器(SCR)。當因靜電荷在接合墊上的電 壓達到一個超過正常操作程度時,則打開SCR,藉以提供 一個放電的低電阻路徑,藉由將此使用於正常操作中的電 路的電路而保護該元件。目前已存在有幾個使用scr的方 法,美國專利第5,369,041號(1)1^¥11〇)係教導一種 ESD保護且在MOS製程中建立SCR之方法。美國專利 、 5, 728, 61 2號(Wei等)係教導一種使用於ESD保護且改 性能,方法,當打開元件時藉由㈣中製造 須需要增加SCR的尺寸。美國專利第5,843,81 3號(^丨等) 係教導另一種改良SCR的ESD保護性能之方法,其亦減少元 件切換噪音’ &兀件亦使用較深接觸窗,當導通時以降低 594968 五、發明說明(2) SCR的電阻。 第二種RSD保護之方法係使用一閘極接地薄氧化層 (GGNMOS)元件,以提供低電阻放電路徑,此係為本發明的 保護方法。現在參閱第1圖,係顯示一種典型GGNM〇s元件 之橫剖面圖,可了解的是,在第丨圖中沒有一個部份是本 發明的習用技藝’更確切的說,此簡單的圖式提供一種結 果,係提供一種改良,其係藉由本發明而克服問題,係提 供一 P型井區或基板10,一閘極氧化層28覆接於p型井區或 基板10上,一多晶矽閘極電極30係覆接於閘極氧化層28 上,提供n+汲極及源極(14及22),一汲極電極18產生電性 連接到汲極14,而一源極電極26產生電性連接到源極22 , 源極電極26係連接到閘極電極30,其兩者均連接到接地 (如第1圖所示)、或連接到1(:使用的最負電壓電位上,對 於此兀件操作的描述,是將源極電極2 6及閘極電極接地。 圖中未顯示的是,亦將p型井區或基板1〇接地。為了要在 使用於1C上的主動NM〇s元件中提供一種較佳的電性接觸, 如第1圖所示,在n+汲極14及源極22的上表面上進行自行 對準矽化處理。遺憾地,由於放電電流局部化,自行對準 石夕化處理會降低GGNM〇s元件的ESD保護性能。美國專利第 6, 1 00, 1 25號(Hu If actor等)係教導一種使用GGNMOS元件之 ESD保護方法,其係修改在元件中的汲極接觸窗,以降低 其傳導性’此會藉由改變輕摻雜汲極(LDD)區及使用一罩 幕而達到,其係防止汲極區的自行對準矽化處理。 崩潰機構係在GGNMOS元件中提供ESD保護,現在再參594968 V. Description of the invention (1) (1) [Technical field to which the invention belongs] The present invention relates to the manufacture of semiconductor devices, and more particularly to an NMOS device formed by electrostatic discharge (ESD) protection during the manufacture of integrated circuits Method. (II) [Previous Technology] Integrated Circuits (ICs) are susceptible to damage known as electrostatic discharge (esd), which occurs when large electrostatic charges accumulate on their ^ ^ pins during component transmission and processing. ^ 1). If the control is improper, ESD will irreparably damage 1C, just like the dissipation of power during the large-scale temperature gradient caused by the discharge in the component structure. Another problem that solves ESD is the silicon controlled rectifier (SCR) connected to 1 (: near the external chat pad). When the voltage on the pad due to static charge reaches a level that exceeds normal operation, the SCR is turned on, thereby Provides a low-resistance path for discharge and protects the element by using this circuit for circuits in normal operation. There are several methods using scr, US Patent No. 5,369,041 (1) 1 ^ ¥ 11. ) Teaches a method of ESD protection and establishing SCR in MOS process. U.S. Patent No. 5,728,61 No. 2 (Wei et al.) Teaches a method for improving the performance of ESD protection. When opening the element, it is necessary to increase the size of the SCR by making it in the core. US Patent No. 5,843,81 3 (^ 丨 etc.) teaches another method to improve the ESD protection performance of SCR, which also reduces component switching noise. &Amp; Elements also use deeper contact windows, which reduces 594968 when turned on 5. Description of the invention (2) Resistance of SCR. The second method of RSD protection is to use a gate-grounded thin oxide layer (GGNMOS) element to provide a low-resistance discharge path. This is the protection method of the present invention. Now referring to Fig. 1, which shows a cross-sectional view of a typical GGNM0s element, it can be understood that none of the parts in Fig. 丨 are conventional techniques of the present invention. More precisely, this simple diagram Provide a result, provide an improvement, overcome the problem by the present invention, provide a P-type well region or substrate 10, a gate oxide layer 28 overlies the p-type well region or substrate 10, a polycrystalline silicon gate The electrode 30 is connected to the gate oxide layer 28 to provide n + drain and source (14 and 22). A drain electrode 18 is electrically connected to the drain 14 and a source electrode 26 is electrically connected. Connected to source 22, source electrode 26 is connected to gate electrode 30, both of which are connected to ground (as shown in Figure 1), or to 1 (: the most negative voltage potential used, for this The description of the operation of the element is to ground the source electrode 26 and the gate electrode. What is not shown in the figure is also to ground the p-type well area or the substrate 10. In order to use active NMs on 1C A better electrical contact is provided in the device, as shown in FIG. 1, on the n + drain 14 and source 22 Self-aligning silicidation treatment is performed on the surface. Unfortunately, due to localization of the discharge current, self-aligning lithography will reduce the ESD protection performance of GGNM0s elements. US Patent No. 6, 1 00, 1 25 (Hu If actor, etc.) teaches an ESD protection method using a GGNMOS device, which modifies the drain contact window in the device to reduce its conductivity. 'This will change the lightly doped drain (LDD) region and use a mask. This is achieved by preventing the self-aligned silicidation of the drain region. The crash mechanism provides ESD protection in the GGNMOS device.
594968 五、發明說明(3) 閱第1圖,現在將描述那些機構。若稍微提高汲極電極i 8 上的電壓超過接地電位時,藉由P型井區1〇及汲極井區所 形成的二極體將為反偏壓,且空乏區將形成於兩者之 間。一第二空乏區存在於源極區12及在閘極30下p型基板 或井區1 0之間,此阻障保留在源極區2 2中的電子,任何流 動的電流是由於在反偏壓沒極/p井區接合中的漏電流。 若增加沒極電極18電壓時,在p型基板或井區1〇及汲 極區之間的空乏區將變寬,將它移動更靠近源極區22。當 在没極電極1 8上的電壓會引起汲極空乏區,以接觸到源極 空乏區時’在兩空乏區之間的連接將會有一個低電阻,此 結果將會是一個非常高的電流,此現象稱之為”穿透",且 結果的電流稱之為’’穿透電流”,一種典型NMOSFET穿透現 象的典型曲線顯示於第2圖,已知没極二極體崩潰的第二 現象係顯示於第2圖,在沒極二極體崩潰之前,實際反偏 壓沒極接合的電流並不會飽和,此是由於當二極體為反偏 t時產生的電洞對,一個論據總是遺落在理想二極體方程 式中。軟崩潰係為由過度電洞對產生的傳導現象。若電場 達到一個發生硬崩潰的關鍵程度時,一個在汲極電壓的微 小增加將會造成一個非常大增加的電流。 第3圖係顯示一個不同源極到汲極井區間距的l對I 圖式,隨著滅少間距,漏電IDS會增加,此會發生是因為如 ^述=兩空乏區互相移得更靠近,而導致從汲極到源極明 .、、、員的場滲透。在源極上的電位阻障係為下降的,導致增 加由源極產生的電子射出,…升Ids增加,此594968 V. Description of the invention (3) With reference to Figure 1, those mechanisms will now be described. If the voltage on the drain electrode i 8 is slightly increased to exceed the ground potential, the diode formed by the P-type well region 10 and the drain well region will be reverse biased, and an empty region will be formed between the two. between. A second empty region exists between the source region 12 and the p-type substrate or well region 10 under the gate 30. This barrier retains the electrons in the source region 22. Any flowing current is due to Leakage current in biased electrodeless / p-well junction. If the voltage of the dead electrode 18 is increased, the empty region between the p-type substrate or the well region 10 and the drain region will become wider, and it will be moved closer to the source region 22. When the voltage on the electrodeless electrode 18 will cause the drain empty region to contact the source empty region, the connection between the two empty regions will have a low resistance, and the result will be a very high Current, this phenomenon is called "penetration", and the resulting current is called "penetration current". A typical curve of a typical NMOSFET penetration phenomenon is shown in Figure 2. It is known that the nonpolar diode collapses. The second phenomenon is shown in Figure 2. Before the pole-diode collapses, the actual reverse-biased pole-junction current will not saturate. This is due to the hole generated when the diode is reverse-biased t Yes, an argument is always left in the ideal diode equation. Soft collapse is a conduction phenomenon caused by excessive hole pairs. If the electric field reaches a critical level for a hard breakdown, a small increase in the drain voltage will cause a very large increase in current. Figure 3 shows a l-to-I pattern with different source-to-drain well spacings. As the gap decreases, the leakage IDS will increase. This happens because, for example, the two empty regions move closer to each other. , Which leads to the field penetration from the drain to the source. The potential barrier on the source is decreasing, which leads to an increase in the emission of electrons generated by the source, ... the Ids increase.
594968 五、發明說明(4) 極導致表面電位降低(DIBL)。再者,增加IDS將會造成空乏 區,以導致穿透。 在某些案例中,於達到穿透電壓之前會發生稱之為回 f (snapback)的不同現象,本發明使用回折以提供ESD保 ”蔓’此現象將會討論於本發明的描詳細說明中。 、二)、【發明内容】 本發明之主要目的,係在於提供一種半導體元件,其 係提供靜電放電(ESD)保護。 ^ 本發明之另一目的,係在於提供一種半導體元件,其 係提供靜電放點(ESD)保護,而無須額外的製程步驟。’、 ^ 本發明之又一目的,係在於提供一種半導體元件,其 係提供靜電放電(ESD)保護,其不需要自行對準矽化理、 阻塞步驟。 ^曰本發明之又一目的,係在於提供一種半導體元件,其 係提供靜電放電(ESD)保護,其不需要一個額外佈 、 進ESD保護。 又 本發明之又一目的,係在於提供一種半導體元件,复 係提供靜電放電(ESD)保護,係具有一個離半導 遠的觸發點。 子股表面很 這些目的係使用一種在GGNMOS元件中井區 J及汲極區下的製程而獲致,修改n井區及p井區推雜八/’、 佈,以致於井區濃度的峰值會在遠離矽表面矽淼: 此會減少在p井區及η井區源極之間的空泛:::生’ 此7卜,在594968 V. Description of the invention (4) The electrode causes a decrease in the surface potential (DIBL). Furthermore, increasing the IDS will result in empty areas, resulting in penetration. In some cases, a different phenomenon called snapback occurs before the penetration voltage is reached. The present invention uses rebates to provide ESD protection. This phenomenon will be discussed in the detailed description of the present invention. (2). [Summary of the Invention] The main object of the present invention is to provide a semiconductor element, which is to provide electrostatic discharge (ESD) protection. ^ Another object of the present invention is to provide a semiconductor element, which is to provide Electrostatic discharge point (ESD) protection without the need for additional process steps. ', ^ Another object of the present invention is to provide a semiconductor device that provides electrostatic discharge (ESD) protection, which does not need to be aligned to the silicon chemical Blocking step. Another object of the present invention is to provide a semiconductor device that provides electrostatic discharge (ESD) protection, which does not require an additional cloth and ESD protection. Yet another object of the present invention is to The purpose is to provide a semiconductor device, the complex system provides electrostatic discharge (ESD) protection, and the system has a trigger point far from the semiconducting surface. It was obtained by a process under the well region J and the drain region in the GGNMOS device, and the n / p region and the p-well region were modified so that the peak concentration of the well region would be far away from the silicon surface: Will reduce the ambiguity between the source of p and η wells ::: 生 '
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反偏壓η井區及p井區間增加的電場,將會造成較^ 生電流。此射出更多電洞到p井區中,以產生一電位/同產 順向偏壓(forward biased)p井區/n井區源極接合,其 果係為有效的一種傳導的雙載子N p n電晶體,在没極 、、Ό 極間的低電阻快速地移除任何靜電荷,在遠離矽表面 生傳導,其係在功率已有效的耗盡處。 _發 (四)、【較佳實施例之詳細說明】 本發明係使用一種ESD保護之方法,其係使用〜 閘極NMOS(GGNMOS)元件,以提供低電阻放電路徑,钱地 區加入到GGNM0S元件的源極及汲極區下,係為了修改n井^ 源極的摻雜分佈。回折係使用於提供ESD保護,隨著v二 增加,因DIBL效應在η井區源極上的電位阻障下降,也會 出現產生在汲極井區空乏區的電洞對,此產生電流係 的且隨著VDS而增加,此結果會導致一個較高電場及一個較 高電洞產生電流,此電洞電流將會注射到p井區中,順向 偏壓p井區/n井區源極接合面。DIBL效應有助於此,其係 ^由降低η井區源極上的電位阻障。一旦p井區“井區源極 接合面係為順向偏壓時,該元件作為NpN電晶體,其汲極 Ϊ ’且▲生一低電阻放電路徑。制習用技藝高級 製程及LDD接合面,此傳導觸發靠近元件表面,其係 在熱傳導不佳處,此表面加熱會導致元件的損壞。 現在參閱第4圖,係顯示本發明GGNM〇s元件之橫剖面 圖,係提供一p型基板或井區1〇,n井區12及2〇係形成於pThe increased electric field in the reverse-biased n-well and p-well zones will cause a relatively large current. This ejects more holes into the p-well area to generate a potential / forward biased p-well area / n-well area source junction, and the effect is an effective conducting double carrier. N pn transistor, the low resistance between the pole, Ό electrode quickly removes any electrostatic charge, and conducts away from the surface of silicon, which is where the power has been effectively depleted. (4), [Detailed description of the preferred embodiment] The present invention uses an ESD protection method, which uses a ~ gate NMOS (GGNMOS) element to provide a low-resistance discharge path, and the money region is added to the GGNM0S element Under the source and drain regions, it is to modify the doping profile of the n-well ^ source. The foldback system is used to provide ESD protection. As v2 increases, the potential barrier on the source of the η well area decreases due to the DIBL effect, and the hole pair generated in the empty area of the drain well area also appears. And with the increase of VDS, this result will cause a higher electric field and a higher hole to generate current. This hole current will be injected into the p-well area, and the source of the p-well area / n-well area will be biased forward. Facing surface. The DIBL effect contributes to this by reducing the potential barrier on the source of the n-well region. Once the "well area source junction surface of p-well area is forward biased, this element acts as an NpN transistor, and its drain Ϊ 'generates a low-resistance discharge path. Advanced manufacturing process and LDD junction surface, This conduction trigger is close to the surface of the element, which is at the place where the heat conduction is not good, and the surface will cause damage to the element. Now referring to FIG. 4, it shows a cross-sectional view of the GGNM0s element of the present invention. Well area 10, n well areas 12 and 20 are formed at p
594968 五、發明說明(6) -- 型基板或井區10中’圖案化一閘極氧化物28,且覆接在p 型基板或井區10及!!井區12及20上。一多晶矽閘極電極3〇 係形成覆接於η井區12及20間的閘極氧化物28上。藉由輕 佈植而形成輕摻雜汲極(LDD)區(15及23),且該輕佈植^ 使用多晶矽閘極電極30作為一罩幕,氧化物間隙壁16及'17 係形成於多晶矽閘極電極3〇的侧壁上,那些氧化物間隙壁 1 6及1 7沿著多晶矽閘極電極3〇,分別形成用於η+源極及汲 極區14及22佈植的罩幕。汲極電極18產生電性連接到汲極 14 ’而源極電極26產生電性連接到源極22。源極電極26係 連接到閘極電極30,且其兩者係連接到接地(如第4圖所 示)、或連接到藉由1C使用的最負電壓電位。對於此元件 操作的描述而言,將源極電極26及閘極電極30接地,ρ型 基板或井區10亦接地(圖中未顯示)。為了要在1(:上的主動 NMOS元件中提供一個較佳的電性接觸窗,如第*圖所示, 在η+及極1 4及源極22上表面上進行自行對準矽化處理。 曲修改η井區12及20及Ρ型基板或井區10 ,以使其峰值 /辰度達到一個從半導體表面〇 · 5到1 · 5 // m之間的點,此峰值 相當於最小汲極空乏寬度,且其係在將會觸發傳導的點 處藉由避免觸發半導體表面,在此較濃峰值濃度點上改 良熱傳導。使用以9 X 1012到5 X 1013i〇ns/ cm2(標稱是2 X l〇13i〇ns/ cm2)之間的劑量及在4〇〇到650KeV(標稱是500KeV) 的佈植能量的磷離子佈植,形成η井區12及2〇,此佈植係 進行於ρ井區佈植前及淺溝槽隔離製程前,使用兩硼離子 佈植而形成ρ型基板或井區1 〇,一個具有在7 χ 1 〇12到4 χ594968 V. Description of the invention (6)-A gate oxide 28 is patterned in the type substrate or well area 10, and is covered on the p-type substrate or well area 10 and !! Wells 12 and 20 are on. A polycrystalline silicon gate electrode 30 is formed on the gate oxide 28 overlying the n-well regions 12 and 20. Lightly doped drain (LDD) regions (15 and 23) are formed by light-weight implantation, and the light-weight implantation uses polycrystalline silicon gate electrode 30 as a mask, and oxide spacers 16 and '17 are formed on On the sidewall of the polysilicon gate electrode 30, those oxide spacers 16 and 17 along the polysilicon gate electrode 30 form a mask for η + source and drain regions 14 and 22, respectively. . The drain electrode 18 is electrically connected to the drain electrode 14 'and the source electrode 26 is electrically connected to the source electrode 22. The source electrode 26 is connected to the gate electrode 30, and both of them are connected to the ground (as shown in FIG. 4), or to the most negative voltage potential used by 1C. For the description of the operation of this element, the source electrode 26 and the gate electrode 30 are grounded, and the p-type substrate or well area 10 is also grounded (not shown in the figure). In order to provide a better electrical contact window in the active NMOS device at 1 (:), as shown in FIG. *, Self-aligned silicidation treatment is performed on the upper surfaces of n +, electrode 14, and source electrode 22. The η well regions 12 and 20 and the P-type substrate or well region 10 are modified so that the peak / degree of the peak reaches a point from the semiconductor surface between 0.5 and 1 · 5 // m. This peak is equivalent to the minimum drain The polar space has a wide width, and it is at the point where the conduction will be triggered to avoid triggering the semiconductor surface, to improve the heat conduction at this thicker peak concentration point. Use 9 X 1012 to 5 X 1013 ions / cm2 (nominal is 2 × 1013inns / cm2) and phosphorus ion implantation at an implantation energy of 400 to 650KeV (nominally 500KeV), forming η well zones 12 and 20, and this planting system Before implantation in the ρ well area and before the shallow trench isolation process, two boron ions are implanted to form a ρ-type substrate or well area 1 〇, one with a range of 7 χ 1 〇12 to 4 χ
594968 五、發明說明(7) 1013ions/ cm2(標稱是j χ 1〇i3i〇ns/ cm2)之間的劑量 400KeV(標稱是30〇KeV)之間的佈植能量,第二p井區佈植 具有一個在1 X 1 〇12到1 χ 1 〇13 i 〇 n s / cm2 (標稱是4 · 5 χ时 之間的劑量及在1〇0及25〇KeV(標稱是15〇KeV) 之間的佈植咸量,這兩個佈植係進行於η井區佈 極氧化物製程前。 俊及間 ^第5圖係顯示本發明之結果,係包括有回折現象,隨 著增加VDS,只有漏電流上升到6 · 2瓦特,一旦達到此臨= 值時’會發生回折現象且立即使、降到4· 3瓦特,會監測 到負電阻區,是由於倍增更多電荷載體有效。修改推^雜分 佈,以致於回折發生於穿透之前。 ^ 第6圖係顯示本發明的η井區摻雜分佈,一個在1 χ ι〇ι? 到5x l〇i8atoms/cm3(標稱是7χ 1〇17)之間的峰值濃度,會在 1C表,的〇·5到l.5/zm(標稱是〇·75 發生。η井區摻雜分 佈係藉由以劑量2 χ i(Pi〇ns/ cm2及在能量5〇〇KeV加上一些臨 限值(Vt)及穿透佈植,以佈植磷離子而形成。第7圖係顯* 示本發明的p井區摻雜分佈,一個在1 X 1 0π到5 χ 1018atoms/ cm3(標稱是7 χ 1 (F)之間的峰值濃度,會在從IC表 面的0.5到1.5//m(標稱是0.6/zm)發生。p井區摻雜分佈係 藉由以劑量1 χ l〇i3ions/ cm2及能量3〇〇KeV、藉由以劑量4· 51 X 1012i〇nS/cra2及能量150KeV、加上一些臨限值(vt)及穿透 佈植,以佈植硼離子而形成。 應該提起在本發明及美國專利第5, 728, 61 2號(Wei等) 之間幾個重要不同之處,Wei等專利係在SCR元件中使用η 594968 五、發明說明(8) 品以擴大傳導體積,此會降低熱光點且改進UD保 井_^發明係應用一GGNM0S元件,且使用修改的11井區及p 壓了二ί分佈,以將傳導從表面移掉,且調整ESD觸發電 的。這些重要的觀點中,兩元件及其操作方法係不同 摘ί中,本發明係使用一種製程,其係n井區加到 分備凡中的源極及汲極區下,修改η井區及ρ井區摻雜 會降柄=致於井區濃度的峰值會在表面遠處發生,此結果 :極Ϊ懕:?及η井區源極之間的空乏阻障’此外,隨著 及北 θ ϋ,一個增加的電場形成在順偏壓η井區没極 &堂、品之間,而導致較高電洞產生電流,此注射出更多 人井區中’以產生一電位,其係將順㈣區/η井 (射此結果為一種具有在汲極(集極)及源極 而、/*間低電阻的傳導雙極ΝΡΝ電晶體,此傳導會在矽表 运二卷生,其係藉由移動靜電荷的功率可有效的消散。 a 然本發明已參考其較佳實施例而被特別地表示並說 :的技藝之人士應瞭解地是各種在形式上及細: 上的改變可在不背離本發明之精神與範疇下為之。 圖號簡單說明: ίο ρ型基板或井區 12 η井區 14 汲極電極 第12頁 594968 五、發明說明(9) 15 輕摻雜汲極(LDD)區 16 氧化物間隙壁 17 氧化物間隙壁 18 汲極電極 2 0 η井區 22 源極 23 輕摻雜汲極(1^0)區 2 6 源極電極 28 閘極氧化物594968 V. Description of the invention (7) The implantation energy between the dose of 400KeV (nominal 30KeV) between 1013ions / cm2 (nominal j χ 1〇i3i〇ns / cm2), the second p-well area The implants have a dose between 1 X 1 〇12 and 1 χ 1 〇13 i 〇ns / cm2 (nominal between 4.5 χ and between 100 and 25 keV (nominal 15 keV ), The two planting systems were carried out before the oxide process in the η well area. Junjima ^ Figure 5 shows the results of the present invention, including the rebate phenomenon, with increasing VDS, only the leakage current rises to 6.2 watts. Once it reaches this value, a reversal phenomenon will occur and it will be immediately reduced to 4.3 watts. The negative resistance area will be detected because it is effective to multiply more charge carriers . Modify the impurity distribution so that the retracement occurs before penetration. ^ Figure 6 shows the doping distribution of the η well area of the present invention, one in the range of 1 x 5 to 8 x 8 atoms / cm3 (nominal It is a peak concentration between 7χ 1〇17), which will occur at 0.5 to 1.5 / zm (nominal 0.75) in Table 1C. The doping distribution in the η well area is determined by the dose 2 χ i (Pi〇ns / cm2 It is formed by implanting phosphorous ions at an energy of 500 KeV plus some threshold (Vt) and penetrating implantation. Figure 7 shows the doping distribution of the p-well region of the present invention, one at 1 X 1 0π to 5 χ 1018 atoms / cm3 (nominal peak concentration between 7 χ 1 (F), will occur from 0.5 to 1.5 // m (nominal 0.6 / zm) from the IC surface. P well area doping The heterogeneous distribution is by a dose of 1 × 10i3ions / cm2 and an energy of 300KeV, by a dose of 4.51 X 1012iSn / cra2 and an energy of 150KeV, plus some threshold (vt) and penetration The implantation is formed by implanting boron ions. Several important differences between the present invention and U.S. Patent No. 5,728,61 2 (Wei et al.) Should be mentioned. The patents of Wei et al. Use η in SCR elements. 594968 V. Description of the invention (8) to increase the conduction volume, which will reduce the hot light point and improve the UD well retention. ^ The invention uses a GGNM0S element, and uses the modified 11 well area and p to reduce the distribution. The conduction is removed from the surface, and the ESD trigger is adjusted. In these important points, the two elements and their operating methods are different. The present invention uses a process, which The n-well area is added to the source and drain regions of the Fenfanfan. Modifying the η-well area and the ρ-well area will reduce the doping = the peak concentration of the well area will occur far away from the surface. This result: Pole?: and the empty barrier between the source of the η well area. In addition, with the north θ ϋ, an increased electric field is formed between the forward bias η well area and the poles, and This causes a higher hole to generate a current, which injects more people into the well area to generate a potential, which will be along the Shun area / η well (the result is a type with a drain (collector) and a source. The low-resistance conductive bipolar NPN transistor is connected between silicon and silicon. This conduction will be generated in the silicon watch, which can be effectively dissipated by moving the power of static charge. a However, the present invention has been specifically shown with reference to its preferred embodiments and said: those skilled in the art should understand that various changes in form and detail can be made without departing from the spirit and scope of the present invention . Brief description of drawing number: ίο ρ-type substrate or well region 12 η well region 14 Drain electrode Page 12 594968 V. Description of the invention (9) 15 Lightly doped drain (LDD) region 16 Oxide spacer 17 Oxide gap Wall 18 Drain electrode 2 0 η well region 22 Source 23 Lightly doped drain (1 ^ 0) region 2 6 Source electrode 28 Gate oxide
30 多晶矽閘極電極章節結束Chapter 30 Polysilicon Gate Electrode Ends
第13頁 594968 圖式簡單說明 第1圖係顯示一種典型的接地閘極NMOS(GGNMOS)元件之橫 剖面圖。 第2圖係顯示一種GGNM0S元件IDS aVDS之圖表。 第3圖係顯示一種不同源極對汲極井區間距之圖表。 第4圖係顯示本發明接地閘極NMOS(GGNMOS)元件之橫剖面 圖。 第5圖係顯示本發明包括有回折(s n a p b a c k )現象之測試結 果。 第6圖係顯示本發明之η井區掺雜分佈。 第7圖係顯示本發明之ρ井區摻雜分佈。Page 13 594968 Brief Description of Drawings Figure 1 shows a cross-sectional view of a typical grounded gate NMOS (GGNMOS) device. Figure 2 shows a diagram of a GGNM0S element IDS aVDS. Figure 3 is a graph showing different well-to-drain well spacings. Fig. 4 is a cross-sectional view showing a grounded gate NMOS (GGNMOS) device according to the present invention. Figure 5 shows the test results of the present invention including the phenomenon of snapback (sn a p b a c k). Figure 6 shows the doping profile of the n-well region of the present invention. Figure 7 shows the doping profile of the p-well region of the present invention.